Imaging lens

ABSTRACT

It is to provide an imaging lens that maintains optical performance and achieves reduction in size and weight. The imaging lens comprises, in order from an object side towards an image surface side, a first lens which is a meniscus lens having a positive power whose convex surface faces the object side, a diaphragm, a second lens which is a meniscus lens having a positive power whose convex surface faces the image surface side, and a third lens which is a biconcave lens having a negative power, wherein the following conditions are to be satisfied; 1.3≧L/fl≧1, 0.8≧f 1 /fl≧0.6, 0.12≧f 1 /f 2 &gt;0, −0.1≧f 1 /f 3 ≧−0.25 (where, L: entire length of the lens system [distance from the surface of the object side of the first lens to the image taking surface [air reduced length]], fl: focal distance of the entire lens system, f 1 : focal distance of the first lens, f 2 : focal distance of the second lens, and f 3 : focal distance of the third lens).

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an imaging lens and, particularly, to an imaging system of three-lens structure, which is capable of reducing the size and weight. The imaging system is used for an image-taking device that uses an image sensor element such as a CCD, CMOS, etc.

2. Description of the Related Art

Recently, there has been an increasing demand for cameras that utilize an image sensor element such as a CCD, CMOS, or the like, which are mounted on a portable computer, a television phone, a portable phone, and a digital camera, for example. It is demanded that a camera such as this is small and light because the camera is required to be mounted on a limited installation space.

Therefore, it is also necessary for the imaging lens system used for such cameras to be small and light, as is the camera. Conventionally, a single lens structure lens system using a single lens and a two-lens structure system that uses two lenses are used as such imaging lens systems.

These imaging lens systems are very advantageous for reducing the size and weight of the lens system. However, these imaging lens systems cannot handle higher definition and higher resolution that is demanded of the imaging lens system in recent years.

Therefore, conventionally, a three-lens lens system using three lenses is utilized to handle higher definition and higher resolution.

As the lens system with three-lens structure aiming for higher definition and higher resolution, there have been known the lens systems disclosed in Patent Literatures 1–4.

[Patent Literature 1] Japanese Patent Unexamined Publication 2005-173298

[Patent Literature 2] Japanese Patent Unexamined Publication 2005-91513

[Patent Literature 3] Japanese Patent Unexamined Publication 2003-322792

[Patent Literature 4] Japanese Patent Unexamined Publication 2004-163786

However, in the lens system in Patent Literature 1, a third lens is a negative lens whose convex surface faces the object side. Therefore, it is difficult to balance between aberration correction and size reduction of the lens system. In addition, the power distribution of first to third lenses and the center radius curvature of both surfaces of the first lens in the lens system in Patent Literature 1 cause the back focus distance to become too long. As a result, the entire length of the lens system becomes too long.

In addition, as in the lens system in Patent Literature 1, the power distribution of the first to third lenses in the lens system in Patent Literature 2 causes the back focus distance to become too long. As a result, the entire length of the lens system becomes too long.

Further, in the lens system in Patent Literature 3, the third lens is a negative lens whose convex surface faces the object side. Therefore, as in the lens system in Patent Literature 1, it is difficult to balance between aberration correction and reducing the size of the lens system. In addition, the power distribution of the first to third lenses in the lens system in Patent Literature 3 causes the overall length of the lens system to become too long. In addition, in the lens system in Patent Literature 3, the back focus distance is short and the third lens has a meniscus shape. Therefore, the last surface in the end of the optical surface protrudes significantly towards the image surface side, thereby causing a problem when various filters and the like are inserted.

Still further, the power distribution of the first, second, and third lenses in the lens system in Patent Literature 4 causes the entire length of the lens system to become too long.

Therefore, the conventional lens systems are still insufficient for maintaining an excellent optical performance, such as high-definition and high-resolution, while actualizing a further reduction in the size and weight (shortening of the entire length) of the lens system itself.

The present invention has been designed in view of the aforementioned problems. The object of the present invention, therefore, is to provide an imaging lens that can maintain an excellent optical performance, while actualizing a further reduction in the size and weight.

SUMMARY OF THE INVENTION

In order to achieve the aforementioned object, the imaging lens according to a first aspect of the present invention is an imaging lens used for forming an image of an object on an image taking surface of a solid-state image sensor element, which comprises, in order from an object side towards an image surface side: a first lens which is a meniscus lens having a positive power whose convex surface faces the object side, a diaphragm, a second lens which is a meniscus lens having a positive power whose convex surface faces the image surface side, and a third lens which is a biconcave lens having a negative power, wherein conditions expressed by each of following expressions (1)–(4) are to be satisfied; 1.3≧L/fl≧1  (1) 0.8≧f1/fl≧0.6  (2) 0.12≧f1/f2≧0  (3) −0.1≧f1/f3≧−0.25  (4)

-   -   where,

L: entire length of the lens system (distance from the surface of the object side of the first lens to the image taking surface [air reduced length])

fl: focal distance of the entire lens system

f₁: focal distance of the first lens

f₂: focal distance of the second lens

f₃: focal distance of the third lens

In the first aspect of the present invention, the first lens is a meniscus lens having a positive power whose convex surface faces the object side, the second lens which is a meniscus lens having a positive power whose convex surface faces the image surface side, a third lens which is a biconcave lens having a negative power, and a diaphragm is disposed between the first lens and the second lens. In addition, the conditions expressed by each of the expressions (1)–(4) are satisfied. With this, it is possible to reduce the size and weight, maintain an excellent optical performance, improve productivity, and secure high telecentricity and back focus distance. In addition, the shape of the second lens allows balance between peripheral areas and the center area.

The productivity herein means not only the productivity for mass-producing imaging lens (for example, moldability, cost, and the like when imaging lens are mass-produced by injection molding), but also easiness of processing, manufacture, etc. of equipment (for example, easiness of processing and the like of a mold used for injection molding), which is used for manufacturing the imaging lens.

An imaging lens according to a second aspect is the imaging lens according to the first aspect, wherein, further, a condition expressed by a following expression (5) is to be satisfied; −1.5≧r ₅ /r ₆≧−10  (5) where,

r₅: center radius curvature of the object side face of the third lens

r₆: center radius curvature of the image surface side face of the third lens

In the second aspect of the invention, further, the expression (5) is satisfied. Thereby, the reduction in size and weight and the maintaining of the optical performance can be compatible with further certainty.

An imaging lens according to a third aspect of the present invention is the imaging lens according to the first or second aspect, wherein, further, a condition expressed by a following expression (6) is to be satisfied; 0.2≧d ₂ /fl≧0.12  (6) where, d₂: distance between the first lens and the second lens on the optical axis

In the third aspect of the invention, further, the expression (6) is satisfied. Thereby, the required back focus distance can be secured while achieving more reduction of the size and weight and improving productivity.

An imaging lens according to a fourth aspect is the imaging lens according to any one of aspects 1–3, wherein, further, a condition expressed by a following expression (7) is to be satisfied; 0.2≧d ₃ /fl≧0.01  (7) where, d₃: center thickness of the second lens

In the fourth aspect of the invention, further, the expression (7) is satisfied. Thereby, further reduction of the size and weight can be achieved and productivity improved.

An imaging lens according to a fifth aspect is the imaging lens according to any one of aspects 1–4, wherein, further, a condition expressed by a following expression (8) is to be satisfied; 0.11≧d ₄ /fl≧0.03  (8) where, d₄: distance between the second lens and the third lens on the optical axis

In the fifth aspect of the invention, further, the expression (8) is satisfied. Thereby, optical performance and productivity can be improved.

An imaging lens according to a sixth aspect is the imaging lens according to any one of aspects 1–5, wherein, further, a condition expressed by a following expression (9) is to be satisfied; 0.25≧r ₁ /r ₂≧0.05  (9) where,

r₁: center radius curvature of the object side face of the first lens

r₂: center radius curvature of the image surface side face of the first lens

In the sixth aspect of the invention, further, the expression (9) is satisfied. Thereby, the required back focus distance can be secured while achieving more reduction of the size and weight and improving productivity.

With the imaging lens according to the first aspect of the present invention, it is possible to achieve an imaging lens that can maintain excellent optical performance, while allowing further reduction in size and weight.

Further, in addition to the effects of the imaging lens according to the first aspect, the imaging lens according to the second aspect can achieve an imaging lens that has more excellent optical performance and is more reduced in size and weight.

Further, in addition to the effects of the imaging lens according to the first or second aspect, the imaging lens according to the third aspect can achieve an imaging lens that has more excellent productivity and is more reduced in size and weight.

Further, in addition to the effects of the imaging lens according to the first to third aspect, the imaging lens according to the fourth aspect can achieve an imaging lens that has more excellent productivity and is more reduced in size and weight.

Further, in addition to the effects of the imaging lens according to the first to fourth aspect, the imaging lens according to the fifth aspect can achieve an imaging lens that has more excellent productivity and optical performance.

Further, in addition to the effects of the imaging lens according to the first to fifth aspect, the imaging lens according to the sixth aspect can achieve an imaging lens that has more excellent productivity and is more reduced in size and weight.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic diagram for showing an embodiment of the imaging lens according to the present invention;

FIG. 2 is a schematic diagram for showing FIRST EXAMPLE of the imaging lens according to the present invention;

FIG. 3 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 2;

FIG. 4 is a schematic diagram for showing SECOND EXAMPLE of the imaging lens according to the present invention;

FIG. 5 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 4;

FIG. 6 is a schematic diagram for showing THIRD EXAMPLE of the imaging lens according to the present invention;

FIG. 7 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 6;

FIG. 8 is a schematic diagram for showing FOURTH EXAMPLE of the imaging lens according to the present invention;

FIG. 9 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 8;

FIG. 10 is a schematic diagram for showing FIFTH EXAMPLE of the imaging lens according to the present invention;

FIG. 11 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 10;

FIG. 12 is a schematic diagram for showing SIXTH EXAMPLE of the imaging lens according to the present invention;

FIG. 13 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 12;

FIG. 14 is a schematic diagram for showing SEVENTH EXAMPLE of the imaging lens according to the present invention;

FIG. 15 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 14;

FIG. 16 is a schematic diagram for showing EIGHTH EXAMPLE of the imaging lens according to the present invention;

FIG. 17 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 16;

FIG. 18 is a schematic diagram for showing NINTH EXAMPLE of the imaging lens according to the present invention;

FIG. 19 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 18;

FIG. 20 is a schematic diagram for showing TENTH EXAMPLE of the imaging lens according to the present invention;

FIG. 21 shows graphs for describing the spherical aberration, astigmatism, and distortion of the imaging lens shown in FIG. 20;

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

An embodiment of the imaging lens according to the present invention will be described hereinafter by referring to FIG. 1.

As shown in FIG. 1, an imaging lens 1 of the embodiment comprises, in order from the object side towards the image surface side, a resin-type first lens 2 which is a meniscus lens having a positive power with its convex surface facing the object side, a diaphragm 3, a resin-type second lens 4 which is a meniscus lens having a positive power with its convex surface facing the image surface side, and a resin-type third lens 5 which is a biconcave lens having a negative power.

Herein, each of the lens surfaces 2 a, 4 a, and 5 a of the first lens 2, the second lens 4, and the third lens 5 on the object side is respectively referred to as first faces 2 a, 4 a, and 5 a of the lenses 2, 4, and 5. The lens surfaces 2 b, 4 b, and 5 b on the image surface side are respectively referred to as second faces 2 b, 4 b, and 5 b of the lenses 2, 4, and 5.

On the second face 5 b side of the third lens 5, there are disposed various filters 6 such as a cover glass, an IR cut filter, and a lowpass filter, and an image taking surface 7 which is a light-receiving surface of an image sensor element such as a CCD or a CMOS, respectively. The various filters 6 may be omitted as required.

Further, in the embodiment, the imaging lens 1 is to satisfy each condition expressed by the following expressions (1)–(4). 1.3≧L/fl≧1.0  (1) 0.8≧f ₁ /fl≧0.6  (2) 0.12≧f ₁ /f ₂≧0  (3) −0.1≧f ₁ /f ₃≧−0.25  (4) where, L in the expression (1) is the entire length of the lens system, i.e. the distance between the first face 2 of the first lens 2 and the image taking surface 7 (air reduced length). fl in the expressions (1) and (2) is the focal distance of the entire lens system. f₁ in the expressions (2) to (4) is the focal distance of the first lens 2. Further, f₂ in the expression (3) is the focal distance of the second lens 4. Still further, f₃ in the expressions (4) is the focal distance of the third lens 5.

When the value of the L/fl exceeds the value (1.3) shown in the expression (1), the entire optical system becomes too large.

At the same time, when the L/fl becomes below the value (1.0) shown in the expression (1), the entire optical system becomes too small. Thus, the productivity is deteriorated and it becomes difficult to maintain the optical performance.

Accordingly, with the embodiment, it becomes possible to reduce the size and weight of the imaging lens while maintaining an excellent optical performance and productivity through setting the value of L/fl to satisfy the expression (1).

It is more preferable for the relation between L and fl to satisfy an expression 1. 3≧L/fl≧1.15.

Further, when the value of f₁/fl exceeds the value (0.8) shown in the expression (2), the back focus distance becomes too long. Thus, it becomes difficult to reduce the size of the optical system.

At the same time, when the value of f₁/fl becomes below the value (0.6), the power of the first lens 2 becomes so strong that the productivity is deteriorated. In addition, it becomes difficult to secure the necessary back focus distance.

Accordingly, with the embodiment, it becomes possible to secure the necessary back focus distance, while more effectively reducing the size and weight and further improving the productivity of the imaging lens 1, through setting the value of f₁/fl to satisfy the expression (2).

It is more preferable for the relation between f₁ and fl to satisfy an expression 0. 8≧f₁/fl≧0.65.

Further, when the value of f₁/f₂ exceeds the value (0.12) shown in the expression (3), the power of the first lens 2 becomes relatively too weak. Thus, it becomes difficult to reduce the size of the optical system. In addition, the power of the first lens 2 and that of the second lens 4 becomes unbalanced, thereby deteriorating the optical performance.

At the same time, when the value of f₁/f₂ is near the value (0) shown in the expression (3), the power of the first lens 2 becomes relatively too strong. Thus, the productivity is deteriorated. In addition, either one of the first lens 2 or the second lens 4 has a negative power. Therefore, the desired optical performance cannot be obtained. Further, the power of the first lens 2 and that of the second lens 4 become unbalanced, thereby deteriorating the optical performance.

Accordingly, with the embodiment, it becomes possible to maintain an excellent optical performance with further certainty, while further reducing the size and weight of the imaging lens 1, through setting the value of f₁/f₂ to satisfy the expression (3).

It is more preferable for the relation between f₁ and f₂ to satisfy an expression 0. 1≧f₁/f₂≧0.07.

Still further, when the value of f₁/f₃ exceeds the value (−0.1) shown in the expression (4), the power of the first lens 2 becomes relatively too strong. Thus, the productivity is deteriorated and the power of the first lens 2 and that of the second lens 4 becomes unbalanced. Thus, the optical performance cannot be maintained.

At the same time, when the value of f₁/f₃ is below the value (−0.25) shown in the expression (4), the power of the third lens 5 becomes relatively too strong. Thus, it becomes difficult to reduce the size and weight of the optical system. In addition, the power of the first lens 2 and that of the third lens 5 become unbalanced, thereby deteriorating the optical performance.

Accordingly, with the embodiment, it is possible to maintain an excellent optical performance with further certainty, while further reducing the size and weight, through setting the value of f₁/f₂ to satisfy the expression (3).

It is more preferable for the relation between f₁ and f₃ to satisfy an expression −0.1≧f₁/f₃≧−0.22.

In addition to the above-described structures, the following expression (5) is satisfied in the embodiment. −1.5≧r ₅ /r ₆≧10  (5) where, r₅ in the expression (5) is the center radius curvature of the first face 5 a of the third lens 5. r₆ is the center radius curvature of the second face 5 b of the third lens 5.

When the value of r₅/r₆ is out of the range of the expression (5), it becomes difficult for the reduction of the size and weight of the entire optical system and the maintaining of an excellent optical performance to be compatible.

Accordingly, with the embodiment, it becomes possible to make compatible the reduction of the size and weight of the entire optical system and the maintaining of an excellent optical performance with further certainly, through satisfying the expression (5).

It is more preferable for the relation between r₅ and r₆ to satisfy an expression −3≧r₅/r₆≧7.

In addition to the above-described structures, the following expression (6) is satisfied in the embodiment. 0.2≧d ₂ /fl≧0.12  (6) where, d₂ in the expression (6) is the distance between the first lens 2 and the second lens 4 on the optical axis 8.

When the value of d₂/fl exceeds the value (0.2) in the expression (6), it becomes difficult to secure the necessary back focus distance. In addition, the height of light ray passing through the second face 5 b of the third lens 5 becomes too high. Thus, the third lens 5 is increased in size and production becomes difficult.

At the same time, when the value of d₂/fl is below the value (0.12) in the expression (6), the back focus distance becomes too long. Thus, it is difficult to reduce the size of the entire optical system. In addition, it becomes difficult to insert the diaphragm that effectively controls the amount of light.

Accordingly, with the embodiment, it becomes possible to more effectively secure the necessary back focus, while further effectively reducing the size and weight of the imaging lens 1 and further improving productivity, through setting the value of d₂/fl to satisfy the expression (6).

It is more preferable for the relation between d₂ and fl to satisfy an expression 0. 18≧d₂/fl≧0.13.

In addition to the above-described structures, the following expression (7) is satisfied in the embodiment. 0.2≧d ₃ /fl≧0.01  (7) where, d₃ in the expression (7) is the center thickness of the second lens 4.

When the value of d₃/fl exceeds the value (0.2) in the expression (7), the back focus distance becomes too long. Thus, it becomes difficult to reduce the size of the entire optical system. In addition, the height of light ray passing through the second face 5 b of the third lens 5 becomes too high. Thus, the third lens 5 is increased in size and production becomes difficult.

At the same time, when the value of d₃/fl is below the value (0.01) in the expression (7), it becomes difficult to produce the second lens 4.

Accordingly, with the embodiment, it becomes possible to more effectively reduce the size and weight of the imaging lens 1 and further improve productivity, through setting the value of d₃/fl to satisfy the expression (7).

It is more preferable for the relation between d₃ and fl to satisfy an expression 0. 18≧d₃/fl≧0.1.

In addition to the above-described structures, the following expression (8) is satisfied in the embodiment. 0.11≧d ₄ /fl≧0.03  (8) where, d₄ in the expression (8) is the distance between the second lens 4 and the third lens 5 on the optical axis 8.

When the value of d₄/fl exceeds the value (0.11) in the expression (8), the height of light ray passing through the second face 5 b of the third lens 5 becomes too high. Thus, the third lens 5 is increased in size and production becomes difficult.

At the same time, when the value of d₄/fl is below the value (0.03) in the expression (8), it becomes difficult to insert the diaphragm that effectively controls the amount of light.

Accordingly, with the embodiment, it becomes possible to further improve the optical performance and the productivity, through setting the value of d₄/fl to satisfy the expression (8).

It is more preferable for the relation between d₄ and fl to satisfy an expression 0.06≧d₄/fl≧0.03.

In addition to the above-described structures, the following expression (9) is satisfied in the embodiment. 0.25≧r ₁ /r ₂≧0.05  (9) where, r₁ in the expression (9) is the center radius curvature of the first face 2 a of the first lens 2. r₂ is the center radius curvature of the second face 2 b of the first lens 2.

When the value of r₁/r₂ exceeds the value (0.25) in the expression (9), the back focus distance becomes too long. Thus, it becomes difficult to reduce the size of the optical system.

At the same time, when the value of r₁/r₂ is below the value (0.05) in the expression (9), the productivity of the first lens 2 is deteriorated. In addition, it becomes difficult to secure the necessary back focus distance.

Accordingly, with the embodiment, it becomes possible to secure the necessary back focus distance, while more effectively reducing the size and weight of the imaging lens and improving the productivity, through setting the value of r₁/r₂ to satisfy the expression (9).

It is more preferable for the relation between r₁ and r₂ to satisfy an expression 0.25≧r₁/r₂≧0.1.

EXAMPLES

Next, EXAMPLES of the present invention will be described by referring to FIG. 2 to FIG. 23.

In the EXAMPLES, F no denotes F number, w denotes a half view angle, and r denotes a center radius curvature. Further, d denotes a distance to the next optical surface, nd denotes the index of refraction to the d line, and vd denotes the Abbe number (d line-based).

k, A, B, C, and D denote each coefficient in a following expression (10). Specifically, the shape of the aspherical surface of the lens is expressed by the following expression provided that the direction of the optical axis 8 is taken as the Z axis, the direction orthogonal to the optical axis 8 as the X axis (the height direction), the traveling direction of light is positive, k is the constant of cone, A, B, C, and D are the aspherical coefficients, and r is the center radius curvature. Z(X)=r ⁻¹ X ²/[1+{1−(k+1)r ⁻² X ²}^(1/2) ]+AX ⁴ +BX ⁶ +CX ⁸ +DX ¹⁰  (10)

In the following EXAMPLES, reference code E used for a numerical value denoting the constant of cone and the aspherical coefficient indicates that the numerical value following E is an exponent having 10 as the base and that the numerical value before E is multiplied by the numerical value denoted by the exponent having 10 as the base. For example, 3.9E-2 denotes 3.9×10⁻².

First Example

FIG. 2 shows FIRST EXAMPLE of the present invention. The imaging lens 1 in FIRST EXAMPLE shown in FIG. 2 is the same imaging lens 1 as that shown in FIG. 1.

The imaging lens 1 of FIRST EXAMPLE was set under the following condition.

(Lens Data) fl = 4.14 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.43 0.95 1.5310 56.0 2 (Second Face of First Lens) 8.81 0.05 3 (Diaphragm) 0.00 0.50 4 (First Face of Second Lens) −0.92 0.60 1.5850 30.0 5 (Second Face of Second Lens) −1.12 0.20 6 (First Face of Third Lens) −40.98 1.10 1.5310 56.0 7 (Second Face of Third Lens) 9.52 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −1.0 3.9E−2 9.7E−3 1.8E−2 −3.2E−2 2 3.0E+1 −6.0E−3 −2.4E−1 2.0E−1 0 4 3.8E−1 1.8E−1 2.1E−1 1.8E−1 0 5 −4.3E−1 1.7E−1 1.1E−1 −2.6E−2 −3.2E−3 6 −8.4E+1 3.3E−2 −9.9E−3 −1.7E−3 6.1E−4 7 1.0E+1 −7.4E−2 1.8E−2 −3.0E−3 2.3E−8 Under such conditions, L/fl = 1.19 was achieved, thereby satisfying the expression (1). f₁/fl = 0.739 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0395 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.2132 was achieved, thereby satisfying the expression (4). r₅/r₆ = −4.21 was achieved, thereby satisfying the expression (5). d₂/fl = 0.133 was achieved, thereby satisfying the expression (6). d₃/fl = 0.145 was achieved, thereby satisfying the expression (7). d₄/fl = 0.048 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.162 was achieved, thereby satisfying the expression (9).

FIG. 3 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the FIRST EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Second Example

FIG. 4 shows SECOND EXAMPLE of the present invention. The imaging lens 1 of SECOND EXAMPLE shown in FIG. 4 was set under the following condition.

(Lens Data) fl = 4.12 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.46 0.95 1.5310 56.0 2 (Second Face of First Lens) 10.00 0.05 3 (Diaphragm) 0.00 0.50 4 (First Face of Second Lens) −0.91 0.62 1.5850 30.0 5 (Second Face of Second Lens) −1.11 0.20 6 (First Face of Third Lens) −50.00 1.10 1.5310 56.0 7 (Second Face of Third Lens) 11.11 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −1.0 3.8E−2 8.3E−3 1.7E−2 −3.2E−2 2 3.4E+1 −5.6E−3 −2.4E−1 2.0E−1 0 4 3.3E−1 1.8E−1 2.1E−1 2.1E−1 0 5 −4.3E−1 1.7E−1 1.1E−1 −2.5E−2 −2.7E−3 6 4.3E+2 3.2E−2 −9.8E−3 −1.6E−3 6.1E−4 7 1.6E+1 −7.3E−2 1.8E−2 −3.0E−3 1.2E−5 Under such conditions, L/fl = 1.21 was achieved, thereby satisfying the expression (1). f₁/fl = 0.750 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0512 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1824 was achieved, thereby satisfying the expression (4). r₅/r₆ = −4.50 was achieved, thereby satisfying the expression (5). d₂/fl = 0.133 was achieved, thereby satisfying the expression (6). d₃/fl = 0.150 was achieved, thereby satisfying the expression (7). d₄/fl = 0.049 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.146 was achieved, thereby satisfying the expression (9).

FIG. 5 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the SECOND EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Third Example

FIG. 6 shows THIRD EXAMPLE of the present invention. The imaging lens 1 of THIRD EXAMPLE shown in FIG. 6 was set under the following condition.

Lens Data fl = 4.09 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.44 0.90 1.5310 56.0 2 (Second Face of First Lens) 11.11 0.05 3 (Diaphragm) 0.00 0.50 4 (First Face of Second Lens) −0.75 0.59 1.5850 30.0 5 (Second Face of Second Lens) −0.94 0.20 6 (First Face of Third Lens) −50.00 1.10 1.5310 56.0 7 (Second Face of Third Lens) 11.77 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −9.8E−1 3.5E−2 4.7E−3 2.9E−2 −5.4E−2 2 −4.7E+1 −1.3E−2 −2.3E−1 1.6E−1 0 4 −1.3E−2 3.2E−1 −1.8E−1 1.4 0 5 −4.4E−1 1.4E−1 2.2E−1 −2.1E−2 −5.0E−3 6 7.3E+2 2.9E−2 −8.2E−3 −1.1E−3 4.9E−4 7 7.2 −7.2E−2 1.8E−2 −3.1E−3 6.1E−5 Under such conditions, L/fl = 1.22 was achieved, thereby satisfying the expression (1). f₁/fl = 0.733 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0681 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1690 was achieved, thereby satisfying the expression (4). r₅/r₆ = −4.25 was achieved, thereby satisfying the expression (5). d₂/fl = 0.134 was achieved, thereby satisfying the expression (6). d₃/fl = 0.144 was achieved, thereby satisfying the expression (7). d₄/fl = 0.049 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.130 was achieved, thereby satisfying the expression (9).

FIG. 7 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the THIRD EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Fourth Example

FIG. 8 shows FOURTH EXAMPLE of the present invention. The imaging lens 1 of FOURTH EXAMPLE shown in FIG. 8 was set under the following condition.

(Lens Data) fl = 3.06 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.08 0.68 1.5310 56.0 2 (Second Face of First Lens) 8.33 0.05 3 (Diaphragm) 0.00 0.40 4 (First Face of Second Lens) −0.56 0.38 1.5850 30.0 5 (Second Face of Second Lens) −0.69 0.15 6 (First Face of Third Lens) −37.50 0.83 1.5310 56.0 7 (Second Face of Third Lens) 8.82 0.75 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −9.8E−1 8.5E−2 −4.3E−2 3.4E−1 −8.8E−1 2 −1.6E+2 −4.4E−2 −8.9E−1 7.0E−1 5.9E−1 4 −1.7E−1 3.3E−1 2.3 4.1E−1 −3.1 5 −4.8E−1 3.7E−1 1.2 −5.7E−1 −6.8E−2 6 0 7.3E−2 −3.1E−2 −9.3E−3 5.1E−3 7 1.7E+1 −1.8E−1 9.0E−2 −2.6E−2 5.7E−4 Under such conditions, L/fl = 1.19 was achieved, thereby satisfying the expression (1). f₁/fl = 0.735 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0118 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1690 was achieved, thereby satisfying the expression (4). r₅/r₆ = −4.25 was achieved, thereby satisfying the expression (5). d₂/fl = 0.147 was achieved, thereby satisfying the expression (6). d₃/fl = 0.123 was achieved, thereby satisfying the expression (7). d₄/fl = 0.049 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.129 was achieved, thereby satisfying the expression (9).

FIG. 9 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the FOURTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Fifth Example

FIG. 10 shows FIFTH EXAMPLE of the present invention. The imaging lens 1 of FIFTH EXAMPLE shown in FIG. 10 was set under the following condition.

(Lens Data) fl = 4.07 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.44 0.90 1.5310 56.0 2 (Second Face of First Lens) 11.11 0.05 3 (Diaphragm) 0.00 0.55 4 (First Face of Second Lens) −0.71 0.50 1.5850 30.0 5 (Second Face of Second Lens) −0.89 0.20 6 (First Face of Third Lens) −40.00 1.05 1.5310 56.0 7 (Second Face of Third Lens) 13.33 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −9.2E−1 3.7E−2 −2.4E−2 6.8E−2 −7.8E−2 2 0 −3.6E−2 −1.8E−1 3.5E−1 9.0E−2 4 −2.4E−1 1.4E−1 6.6E−1 −1.5E−1 −1.0E−1 5 −6.0E−1 1.6E−1 2.9E−1 −7.9E−2 −1.6E−2 6 0 3.5E−2 −9.7E−3 −1.6E−4 2.1E−4 7 −7.1E+2 −7.1E−2 2.1E−2 −3.6E−3 7.7E−5 Under such conditions, L/fl = 1.19 was achieved, thereby satisfying the expression (1). f₁/fl = 0.737 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0302 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1610 was achieved, thereby satisfying the expression (4). r₅/r₆ = −3.00 was achieved, thereby satisfying the expression (5). d₂/fl = 0.147 was achieved, thereby satisfying the expression (6). d₃/fl = 0.123 was achieved, thereby satisfying the expression (7). d₄/fl = 0.049 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.130 was achieved, thereby satisfying the expression (9).

FIG. 11 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the FIFTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Sixth Example

FIG. 12 shows SIXTH EXAMPLE of the present invention. The imaging lens 1 of SIXTH EXAMPLE shown in FIG. 12 was set under the following condition.

(Lens Data) fl = 4 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.44 0.90 1.5310 56.0 2 (Second Face of First Lens) 11.11 0.05 3 (Diaphragm) 0.00 0.70 4 (First Face of Second Lens) −0.69 0.50 1.5850 30.0 5 (Second Face of Second Lens) −0.87 0.31 6 (First Face of Third Lens) −40.00 1.00 1.5310 56.0 7 (Second Face of Third Lens) 20.00 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −9.6E−1 3.6E−2 −4.8E−2 1.0E−2 −8.7E−2 2 1.5E+1 −4.0E−2 −1.4E−1 6.4E−2 1.1E−1 4 −3.4E−1 9.7E−2 7.3E−1 −1.7E−1 −2.6E−2 5 −6.8E−1 1.2E−1 2.9E−1 −5.6E−2 −2.8E−2 6 −1.7E+3 4.7E−2 −1.2E−2 7.6E−4 4.1E−5 7 −8.0E+1 −7.5E−2 2.3E−2 −4.5E−3 1.6E−4 Under such conditions, L/fl = 1.19 was achieved, thereby satisfying the expression (1). f₁/fl = 0.750 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0164 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1207 was achieved, thereby satisfying the expression (4). r₅/r₆ = −2.00 was achieved, thereby satisfying the expression (5). d₂/fl = 0.188 was achieved, thereby satisfying the expression (6). d₃/fl = 0.125 was achieved, thereby satisfying the expression (7). d₄/fl = 0.078 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.130 was achieved, thereby satisfying the expression (9).

FIG. 13 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the SIXTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Seventh Example

FIG. 14 shows SEVENTH EXAMPLE of the present invention. The imaging lens 1 of SEVENTH EXAMPLE shown in FIG. 14 was set under the following condition.

(Lens Data) fl = 4.06 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.47 0.92 1.5310 56.0 2 (Second Face of First Lens) 12.75 0.05 3 (Diaphragm) 0.00 0.56 4 (First Face of Second Lens) −0.68 0.46 1.5850 30.0 5 (Second Face of Second Lens) −0.85 0.15 6 (First Face of Third Lens) −40.80 1.12 1.5310 56.0 7 (Second Face of Third Lens) 20.40 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −9.6E−1 3.3E−2 −1.9E−2 5.4E−2 −6.5E−2 2 0 −3.9E−2 −1.9E−1 1.1E−1 8.1E−3 4 −3.9E−1 1.2E−1 1.0 −1.0 2.9E−1 5 −7.8E−1 1.3E−1 4.4E−1 −2.7E−1 4.1E−2 6 0 4.7E−2 −2.2E−2 −4.8E−3 −4.0E−4 7 0 −9.5E−2 3.3E−2 −7.2E−2 5.0E−4 Under such conditions, L/fl = 1.20 was achieved, thereby satisfying the expression (1). f₁/fl = 0.744 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0019 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1192 was achieved, thereby satisfying the expression (4). r₅/r₆ = −1.95 was achieved, thereby satisfying the expression (5). d₂/fl = 0.150 was achieved, thereby satisfying the expression (6). d₃/fl = 0.113 was achieved, thereby satisfying the expression (7). d₄/fl = 0.037 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.115 was achieved, thereby satisfying the expression (9).

FIG. 15 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the SEVENTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Eighth Example

FIG. 16 shows EIGHTH EXAMPLE of the present invention. The imaging lens 1 of EIGHTH EXAMPLE shown in FIG. 16 was set under the following condition.

(Lens Data) fl = 4.08 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.44 0.90 1.5310 56.0 2 (Second Face of First Lens) 11.11 0.05 3 (Diaphragm) 0.00 0.56 4 (First Face of Second Lens) −0.87 0.60 1.5850 30.0 5 (Second Face of Second Lens) −1.08 0.20 6 (First Face of Third Lens) −50.00 1.10 1.5310 56.0 7 (Second Face of Third Lens) 11.77 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −9.8E−1 3.5E−2 −4.7E−3 2.9E−2 −5.4E−2 2 −4.7E+1 −1.3E−2 −2.3E−1 1.6E−1 0 4 1.9E−1 1.7E−1 2.0E−1 2.2E−1 0 5 −4.4E−1 1.6E−1 1.3E−1 −1.8E−2 −5.0E−3 6 7.3E+2 2.9E−2 −8.2E−3 −1.1E−3 4.9E−4 7 7.2 −7.2E−2 1.8E−2 −3.1E−3 6.1E−5 Under such conditions, L/fl = 1.21 was achieved, thereby satisfying the expression (1). f₁/fl = 0.735 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0208 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1690 was achieved, thereby satisfying the expression (4). r₅/r₆ = −4.25 was achieved, thereby satisfying the expression (5). d₂/fl = 0.135 was achieved, thereby satisfying the expression (6). d₃/fl = 0.147 was achieved, thereby satisfying the expression (7). d₄/fl = 0.049 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.130 was achieved, thereby satisfying the expression (9).

FIG. 17 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the EIGHTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Ninth Example

FIG. 18 shows NINTH EXAMPLE of the present invention. The imaging lens 1 of NINTH EXAMPLE shown in FIG. 18 was set under the following condition.

(Lens Data) fl = 4.06 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.43 0.72 1.5310 56.0 2 (Second Face of First Lens) 7.69 0.02 3 (Diaphragm) 0.00 0.68 4 (First Face of Second Lens) −0.84 0.55 1.5850 30.0 5 (Second Face of Second Lens) −1.00 0.18 6 (First Face of Third Lens) −60.61 1.15 1.5310 56.0 7 (Second Face of Third Lens) 10.99 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −8.4E−1 3.7E−2 −2.5E−2 7.0E−2 −9.0E−2 2 0 −3.3E−2 −6.7E−2 −5.7E−2 0 4 −4.8E−2 4.8E−2 4.4E−1 −6.9E−2 0 5 −5.5E−1 1.1E−1 1.0E−1 8.0E−2 −5.1E−2 6 0 2.2E−2 −8.6E−3 1.3E−3 −3.3E−5 7 −5.6E−2 −6.5E−2 1.6E−2 −3.3E−2 2.0E−4 Under such conditions, L/fl = 1.21 was achieved, thereby satisfying the expression (1). f₁/fl = 0.660 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0834 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1545 was achieved, thereby satisfying the expression (4). r₅/r₆ = −5.52 was achieved, thereby satisfying the expression (5). d₂/fl = 0.172 was achieved, thereby satisfying the expression (6). d₃/fl = 0.135 was achieved, thereby satisfying the expression (7). d₄/fl = 0.044 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.186 was achieved, thereby satisfying the expression (9).

FIG. 19 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the NINTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

Tenth Example

FIG. 20 shows TENTH EXAMPLE of the present invention. The imaging lens 1 of TENTH EXAMPLE shown in FIG. 20 was set under the following condition.

(Lens Data) fl = 3.88 mm, F no = 2.8 Face Number r d nd vd (Object Point) 1 (First Face of First Lens) 1.37 0.69 1.5310 56.0 2 (Second Face of First Lens) 7.41 0.02 3 (Diaphragm) 0.00 0.65 4 (First Face of Second Lens) −0.81 0.53 1.5850 30.0 5 (Second Face of Second Lens) −0.96 0.17 6 (First Face of Third Lens) −66.67 1.10 1.5310 56.0 7 (Second Face of Third Lens) 11.11 1.00 8 (First Face of Cover Glass) 0.00 0.30 1.5168 64.2 9 (Second Face of Cover Glass) 0.00 (Image Surface) Face Number k A B C D 1 −8.4E−1 4.2E−2 −3.0E−2 9.2E−2 −1.3E−1 2 0 −4.3E−2 −5.9E−2 −1.0E−1 0 4 −8.5E−2 4.8E−2 5.5E−1 −1.1E−1 0 5 −5.7E−1 1.3E−1 1.2E−1 1.1E−1 −6.6E−2 6 0 2.5E−2 −1.5E−2 1.6E−3 4.7E−4 7 −1.0E+2 −6.8E−2 1.9E−2 −5.2E−3 3.8E−4 Under such conditions, L/fl = 1.21 was achieved, thereby satisfying the expression (1). f₁/fl = 0.781 was achieved, thereby satisfying the expression (2). f₁/f₂ = 0.0956 was achieved, thereby satisfying the expression (3). f₁/f₃ = −0.1705 was achieved, thereby satisfying the expression (4). r₅/r₆ = −6.00 was achieved, thereby satisfying the expression (5). d₂/fl = 0.173 was achieved, thereby satisfying the expression (6). d₃/fl = 0.137 was achieved, thereby satisfying the expression (7). d₄/fl = 0.044 was achieved, thereby satisfying the expression (8). r₁/r₂ = 0.185 was achieved, thereby satisfying the expression (9).

FIG. 21 shows the spherical aberration, astigmatism, and distortion of the imaging lens 1 of the TENTH EXAMPLE.

According to the result, each of the spherical aberration, astigmatism, distortion, and lateral aberration was satisfied. It can be seen from the result that a sufficiently excellent optical property can be obtained.

The present invention is not limited to the above-described embodiments and EXAMPLES, and various modifications are possible as required. 

1. An imaging lens used for forming an image of an object on an image taking surface of a solid-state image sensor element, comprising: in order from an object side towards an image surface side, a first lens which is a meniscus lens having a positive power whose convex surface faces the object side, a diaphragm, a second lens which is a meniscus lens having a positive power whose convex surface faces the image surface side, and a third lens which is a biconcave lens having a negative power, wherein conditions expressed by each of following expressions (1)–(4) are to be satisfied; 1.3≧L/fl≧1  (1) 0.8≧f ₁ /fl≧0.6  (2) 0.12≧f ₁ /f ₂≧0  (3) −0.1≧f ₁ /f ₃≧−0.25  (4) where, L: entire length of the lens system (distance from the surface of the object side of the first lens to the image taking surface [air reduced length]) fl: focal distance of the entire lens system f₁: focal distance of the first lens f₂: focal distance of the second lens f₃: focal distance of the third lens.
 2. The imaging lens according to claim 1, wherein, further, a condition expressed by a following expression (5) is to be satisfied; −1.5≧r ₅ /r ₆≧10  (5) where, r₅: center radius curvature of the object side face of the third lens r₆: center radius curvature of the image surface side face of the third lens.
 3. The imaging lens according to claim 1, wherein, further, a condition expressed by a following expression (6) is to be satisfied; 0.2≧d ₂ /fl≧0.12  (6) where, d₂: distance between the first lens and the second lens on the optical axis.
 4. The imaging lens according to claim 1, wherein, further, a condition expressed by a following expression (7) is to be satisfied; 0.2≧d ₃ /fl≧0.01  (7) where, d₃: center thickness of the second lens.
 5. The imaging lens according to claim 1, wherein, further, a condition expressed by a following expression (8) is to be satisfied; 0.11≧d ₄ /fl≧0.03  (8) where, d₄: distance between the second lens and the third lens on the optical axis.
 6. The imaging lens according to claim 1, wherein, further, a condition expressed by a following expression (9) is to be satisfied; 0.25≧r ₁ /r ₂≧0.05  (9) where, r₁: center radius curvature of the object side face of the first lens r₂: center radius curvature of the image surface side face of the first lens. 